TJ-II:Electron Bernstein Wave Heating: Difference between revisions
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which has been used successfully in the W7-AS and H-J | which has been used successfully in the W7-AS and H-J | ||
stellarators, is being explored. | stellarators, is being explored. | ||
<ref>A. Fernández et al., ''The design of an electron Bernstein wave heating | <ref>[http://www.new.ans.org/store/j_572 A. Fernández et al., ''The design of an electron Bernstein wave heating system for the TJ-II stellarator,'' Fusion Sci. Tech. '''46''', pp. 335-341 (2004)]</ref> | ||
system for the TJ-II stellarator,'' Fusion Sci. Tech. '''46''', pp. 335-341 | |||
(2004)</ref> | |||
It offers a way of | It offers a way of | ||
overcoming the cut-off density limit associated with ECRH | overcoming the cut-off density limit associated with ECRH | ||
Revision as of 09:10, 5 August 2009
In TJ-II, the possibility of achieving high-density plasmas using Electron Bernstein Wave Heating (EBWH), which has been used successfully in the W7-AS and H-J stellarators, is being explored. [1] It offers a way of overcoming the cut-off density limit associated with ECRH methods (1.7×1019 m-3 in TJ-II). Preliminary studies highlighted several promising EBWH first harmonic schemes, i.e. at 28 GHz. [2]
References
- ↑ A. Fernández et al., The design of an electron Bernstein wave heating system for the TJ-II stellarator, Fusion Sci. Tech. 46, pp. 335-341 (2004)
- ↑ F. Castejón et al., Electron Bernstein wave heating calculations for TJII plasmas, Fusion Sci. Tech. 46, pp. 327-334 (2004)